EP0265956A2 - Méthode pour corriger la déviation de position occasionnée par un changement du champ magnétique statique dans un appareil d'imagerie par RMN - Google Patents

Méthode pour corriger la déviation de position occasionnée par un changement du champ magnétique statique dans un appareil d'imagerie par RMN Download PDF

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Publication number
EP0265956A2
EP0265956A2 EP87115930A EP87115930A EP0265956A2 EP 0265956 A2 EP0265956 A2 EP 0265956A2 EP 87115930 A EP87115930 A EP 87115930A EP 87115930 A EP87115930 A EP 87115930A EP 0265956 A2 EP0265956 A2 EP 0265956A2
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Prior art keywords
magnetic field
nmr
frequency
applying
gradient magnetic
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EP87115930A
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German (de)
English (en)
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EP0265956B1 (fr
EP0265956A3 (en
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Hiroshi Nishimura
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Hitachi Healthcare Manufacturing Ltd
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Hitachi Medical Corp
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Publication of EP0265956A3 publication Critical patent/EP0265956A3/en
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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00—Arrangements or instruments for measuring magnetic variables
    • G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/44—Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
    • G01R33/48—NMR imaging systems
    • G01R33/483—NMR imaging systems with selection of signals or spectra from particular regions of the volume, e.g. in vivo spectroscopy
    • G01R33/4833—NMR imaging systems with selection of signals or spectra from particular regions of the volume, e.g. in vivo spectroscopy using spatially selective excitation of the volume of interest, e.g. selecting non-orthogonal or inclined slices
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00—Arrangements or instruments for measuring magnetic variables
    • G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/44—Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
    • G01R33/48—NMR imaging systems
    • G01R33/54—Signal processing systems, e.g. using pulse sequences ; Generation or control of pulse sequences; Operator console
    • G01R33/56—Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution
    • G01R33/565—Correction of image distortions, e.g. due to magnetic field inhomogeneities
    • G01R33/56563—Correction of image distortions, e.g. due to magnetic field inhomogeneities caused by a distortion of the main magnetic field B0, e.g. temporal variation of the magnitude or spatial inhomogeneity of B0

Definitions

  • This invention relates to a nuclear magnetic resonance (NMR) imaging method and more particularly to a method for absorbing time change of the static magnetic field in an NMR imaging device to remove the positional deviation of an NMR image on measurement thereof.
  • NMR nuclear magnetic resonance
  • An NMR imaging (simply referred to as MRI) is a system for imaging anatomic or biochemical information based on the protons or other nuclides.
  • the image therein includes a nuclear spin density image itself, the nuclear spin density image enhanced with a longitudinal relaxation time T1 or lateral relaxation time T2, and T1 calculated image or T2 calculated image.
  • the NMR imaging makes it possible to see, as images, the parameters related with tissues, which provides medically important information in judging the abnormality of the tissue.
  • an object to be examined is placed in a static magnetic field, which can be generated by a permanent magnet, resistive magnet or superconductive magnet, and is irradiated with RF (radio frequency) pulses (or selectively excited pulses). Subsequently, the resonance signals emitted from the object are received.
  • the NMR imaging is carried out in such a way that the NMR signals are measured under the condition where a gradient magnetic field is applied and thereafter the resultant images are reconstructed. More specifically, the object is irradiated with the RF pulses under the condition where the gradient magnetic field is applied and the NMR signals produced from the examination region of the object are encoded as spatial information.
  • the gradient magnetic field is employed for encoding the space for the reason why a nuclear resonance frequency ⁇ is in a linear relation with the magnetic field. Specifically, if the gradient magnetic field remains spatially linear, the spatial position of the examination region is linearly related with the resonance frequency.
  • the position information of the object can be obtained by only Fourier transforming the NMR signals, which are time information, so as to be changed into a frequency axis. This can be employed to reconstruct the image.
  • the problem of the position deviation can be considered individually in a two-dimentional image and in a slice direction perpendicular thereto.
  • the NMR imaging device for medical use takes several minutes or more for normal measurement and thus uses a multi-slice technique to provide a number of images through one measurement.
  • a number of images can be obtained by irradiating object slices with selectively excited pulses at the center frequency corresponding to the object slice in a condition where the gradient magnetic field is applied. Then, if the static magnetic field is being varied, the signal at different slice position from the predetermined slice position will be measured. This results in undesired anatomic position deviations.
  • the center frequency corresponding to a prescribed slice position is ⁇ 0, that is, the center frequency decided by the static magnetic field at the isocenter is ⁇ 0.
  • the above center frequency is varied to ⁇ 1 by the change of the static magnetic field due to the ambient temperature.
  • the slice position is S0.
  • the center frequency ⁇ 1 at the isocenter becomes a central point of the gradient magnetic field. If ⁇ 1 > ⁇ 0, the slice position corresponding to the center frequency ⁇ 0 is S1 which is a position leftwardly shifted from S0 in Fig. 1.
  • the above phenomenon will be explained in detail with reference to Figs. 2 and 3.
  • the detection of NMR signals is defined as taking a difference signal between the frequency of a received signal and a predetermined center frequency. It is now assumed that the predetermined center frequency ⁇ 1 is different from the proton resonance frequency ⁇ 0 decided by the static magnetic field at the isocenter in an imaging space.
  • Fig. 2 schematically shows a time sequence in a typical spin echo measurement.
  • RF shows timings of irradiating RF signals and its envelope for selective excitation
  • G z shows timings of applying a gradient magnetic field in the slice direction
  • G y shows timings of applying a gradient magnetic field in the direction of phase encoding and the amplitudes thereof varied
  • G x shows timings of applying a gradient magnetic field in the direction of frequency encoding.
  • Signal shows NMR signals to be measured; and the lowest stage shows plural sections of the time-sequence.
  • the 90 degree selective excitation pulse is irradiated onto an object and also the slice direction gradient magnetic field is applied.
  • the gradient magnetic field in the phase encode direction is applied to provide the rotation of a nuclear spin dependent upon the position in the y direction.
  • any signal is not applied.
  • the 180 degree selective excitation pulse is irradiated and also the gradient magnetic field in the slice direction is applied.
  • the gradient magnetic field in the frequency encode direction is applied and the NMR signal is measured.
  • the frequency must be essentially returned to the proton resonance frequency which is decided by the static magnetic field intensity at the isocenter in an imaging space.
  • the predetermined center frequency ⁇ 1 which is to be essentially equal to ⁇ 0 is different from ⁇ 0, the position deviation will be measured in the direction of frequency encoding. More specifically, as already mentioned, the NMR signal is measured as the difference frequency from the center frequency so that the center of the resultant image corresponds to the frequency ⁇ 0.
  • will occur in the frequency encode direction on the two dimentional image (see Fig. 3).
  • the direction of deviation depends upon if the frequency encode gradient magnetic field is positive or negative in the x-axis direction.
  • this magnetic field locking technique has the following disadvantages. If the magnet having a negative temperature coefficient is used as in the permanent magnet NMR imaging device, the current flowing through the shim or correcting coil generates heat, thus further decreasing the static magnetic field, which requires the current to be further increased. Such a vicious circle can be cut by slightly cancelling the static magnetic field generated in the permanent magnet by always passing the current through the shim coil. Specifically, if the current to be passed through the coil is decreased when the ambient temperature is increased and the static magnetic field generated by the permanent magnet is decreased, the static magnetic field can be restored to the assumed magnetic field at the center of imaging and also the current generation is decreased due to the decreased current.
  • An object of this invention is to provide an NMR imaging method which is capable of readily correcting position deviation without using shim coils for correct­ing static magnetic field.
  • this invention is characterized in that prior to imaging, the NMR signals measured without applying to an object to be examined a gradient magnetic field in the phase encode direction and gradient magnetic field in the frequency encode direction are Fourier-transformed to detect a static magnetic field intensity, thereby following a center frequency to remove any position deviation in imaging.
  • FIG. 4 showing an entire arrangement of an NMR imaging device according to this invention which provides tomograms using NMR phenomena, it essentially consists of an static magnetic field generating magnet 10, a central processing unit (CPU) 11, a sequencer 12, a transmitter unit 13, a receiver unit 14, a gradient magnetic field unit 15 and a signal processing unit 16.
  • the static magnetic field generating magnet 10 serves to generate, around an object 2 to be examined (e.g. human body), a strong and uniform static magnetic field in the direction of a body axis or in the direction perpendicular thereto.
  • Magnetic field generating means of permanent magnet, resistive magnet or superconductive magnet is arranged in the space having a certain expanse around the object.
  • the sequencer 12 which is operated under the control by the CPU 11, serves to transfer several instructions necessary for collecting the data of tomograms of the object 2, at certain timings, to the transmitter unit 13, the gradient magnetic field generating unit 15 and the receiver unit 14.
  • the transmitter unit 13 includes a high frequency oscillator 17, a modulator 18, a video frequency amplifier 19 and radio frequency transmitter coil 20a.
  • high frequency pulses are first generated from the radio frequency oscillator 17; the radio frequency pulses thus generated are amplitude-modulated by the modulator 18 in accordance with an instruction signal from the sequencer 12 so as to be selectively excited, the radio frequency pulses amplitude-modulated are amplified by the high frequency amplifier 19 and thereafter supplied to the radio frequency coil 20 arranged in proximity to the periphery of the object 2.
  • radio frequency electromagnetic waves are irradiated to the object 2.
  • the receiver unit 14 After a specific section of the object 2 is excited, the supply of the radio frequency pulses is stopped. Then, after a certain time, weak electromagnetic waves are emitted from the object 2.
  • the receiver unit 14 includes a radio frequency receiver coil 20b, an amplifier 21, a quadrature phase detector 22, and an A/D converter 23.
  • the weak electromagnetic waves emitted from the object 2 are detected by the radio frequency receiver coil 20b, which is arranged in proximity to the periphery of the object 2, the electromagnetic waves detected are transferred to the A/D converter 23 through the amplifier 21 and the quadrature phase detector 22, thus being converted into digital amounts.
  • the timing of signal processing is such that the outputs from the quadrature phase detector 22 are collected as two series of sampling data in accordance with an instruction from the sequencer 12 and the data collected are transferred to the signal processing unit 16.
  • the gradient magnetic field generating unit 15 consists of gradient magnetic field coils 24 which are arranged to generate the magnetic fields having the gradients in respectively orthogonal three axis X, Y and Z directions and a gradient magnetic field power supply 25 which drives the respective coils 24.
  • the gradient magnetic field power supply 25 for the respective coils in accordance with an instruction from the sequencer to apply the gradient magnetic fields G X , G Y and G Z in the three X, Y, and Z directions to the object 2.
  • the tomogram section of the object 2 can be optionally set up to the arbitrary angle to the axis.
  • the signal processing unit 16 essentially consists of the CPU 11, a recording device such as a magnetic disk 26, a magnetic tape 27, etc., and a display device 28 such as a CRT.
  • the NMR signals provided in the CPU 11 are subjected to the processing such as Fourier transform, phase correction, etc. to create a reconstructed image, thereby imaging the signal intensity distribution on a certain tomogram section or the distribution of plural signal groups subjected to any suitable arithmetic operation to be shown on the display device 28.
  • the transmitter and receiver coils 20a, 20b and the gradient magnetic field coils 24 are located in the imaging space of the static magnetic field generating magnet 10 arranged in the space surrounding the object 2.
  • a rare-earth magnet (Nd-Fe-B), which has been recently used, is the highest in the maximum energy product but also has a high temperature coefficient. It has a so-called negative temperature coefficient that when the ambient temperature is increased, the generated static magnetic field is weakened.
  • One example thereof has a temperature co­efficient as great as -1000 ppm/°C. With this temperature coefficient, when the ambient temperature is increased by 1°C, the static magnetic field is weakened by 1000 ppm which corresponds to 1 Gauss for the static magnetic field of 1000 Gauss, for example. In this case, to what extent the position deviation occurs on the image will be described below.
  • the cause of the position deviation resides in that although the static magnetic field in the object imaging space has changed due to temperature change, the center frequency for the assumed central magnetic field in the center of imaging space has not been changed correspondingly.
  • ⁇ ⁇ B
  • ⁇ a gyromagnetic ratio of a noticed nuclear spin.
  • ⁇ 4257.59 ⁇ 2 ⁇ (rad/sec)/Gauss
  • the NMR frequency is 4.25759 MHz. 1 Gauss corresponds to 4.26 KHz.
  • the center frequency following technique in accordance with this invention is to make zero the difference frequency mentioned above and more specifically to always monitor the change in a static magnetic field intensity to cause the center frequency to follow it.
  • Fig. 6 shows a time sequence of measuring a center frequency.
  • reference symbols has the same meanings as in Fig. 3.
  • the selectively excitation waveform is the amplitude-modulated sine wave signals at the frequency of ⁇ 0.
  • the amplitude-modulated, 90 degree selective excitation radio frequency pulse at the frequency ⁇ 0 is irradiated onto the object and also the gradient magnetic field in the slice direction G z is applied.
  • any signal is not applied to the object.
  • the amplitude-modulated 180 degree selective excitation radio frequency pulse is irradiated to the object and also the gradient magnetic field in the slice direction G z is applied.
  • the nuclear spin on a specific tomogram section is reversed in a rotating coordinate system.
  • the NMR signal is measured without applying any gradient magnetic field.
  • the Fourier transforms thereof don't include the position information relative to the nuclear spin on the excited tomogram section, and constitute a spectrum to be used in a spectrocopy region.
  • the abscissa in the Fourier transformed region is frequency.
  • Fig. 7(a) illustrates the NMR signal measured in the manner mentioned above, with the abscissa being time.
  • Fig. 7(b) illustrates the Fourier transform thereof, with the abscissa being frequency.
  • the center frequency ⁇ 1 decided by a static magnetic field intensity is different from the one for the assumed center frequency ⁇ 0, as seen from Fig. 7(b) the peak of the spectrum is not located at the origin of the spectrum coordinate but at the position deviated by ⁇ 1 - ⁇ 0. Therefore, in order that the resonance frequency coincides with the center frequency, the above difference frequency ⁇ 1 - ⁇ 0 is added to the previously assumed center frequency ⁇ 0 thereby to provide a new center frequency.
  • Step 101 a suitable central frequency ⁇ 0 is set (Step 101).
  • Step 106 If the peak value is equal to the noise level or less (Step 106, "NO"), the previously set frequency ⁇ 0 is shifted to another frequency range (Step 108). Even when the frequency range is thus changed, the peak value may not be obtained within the specified frequency range (Step 109, "NO"). Then, the processing is terminated under the judgement of the presence of abnormality of the measurement system (i.e. abnormal termination) (Step 110). If not so (Step 109, "YES”) the processing is returned to the step of measuring the NMR signal.
  • Fig. 9 shows inner component blocks in the CPU of Fig. 4 along their processing flowchart.
  • Fig. 4 shows the main components of the entire NMR imaging device
  • Fig. 9 shows the operations of the main components in the embodiment of this invention in their flowchart and so plural blocks with the same reference number are included in Fig. 4.
  • the blocks in Fig. 9 which are not shown in Fig. 4 are included in the CPU 11, magnetic disk 26 or magnetic tape 27.
  • an assumed center frequency ⁇ 0 is set in the radio frequency oscillator 17 by a center frequency set up I/F (interface) 30.
  • the sequencer 12 is actuated by a measurement starting I/F 31 to start the measure­ment of NMR signal.
  • the gradient magnetic field in the frequency encode direction and the gradient magnetic field in the phase encode direction are not applied.
  • the NMR signals digitized by the A/D converter 23 during the measurement are stored in a one-dimensional buffer memory 33 through a data collection circuit 32.
  • the contents of the one-dimensional buffer memory are Fourier-transformed by a FFT (fast Fourier transform) arithmetic device 34.
  • FFT fast Fourier transform
  • the resultant data thereof is transferred to a one-­dimensional buffer memory 35. Since the measured data are complex data each consisting of a real part and an imaginary part, the absolute values thereof are calculated by a complex absolute value arithmetic device 36 and the absolute values are transferred to a one-dimensional buffer memory 37. The peak value among the absolute values is taken out by a peak detection arithmetic device 38 and loaded in a register 39.
  • the value loaded in the register 39 are compared with a preset noise level by a comparator 40. If it is equal to or less than the noise level, it is set to another frequency range under the judgement that the peak has not been properly detected. Concretely, this is carried out by adding a certain increment to or subtracting it from the present center frequency in the frequency range set I/F 30. Whether or not the frequency range is a preset frame is judged in a com­parator 42. If this is negative, the processing is abnormal-terminated. If the frequency range is within the frame, the processing is returned to the center frequency set I/F 30 to start again the detection of the peak value mentioned above. Incidentally, a frame of specifying the frequency range to be used is preset in the comparator 42.
  • a frequency difference from the center frequency is calculated by a difference frequency calculating circuit 43.
  • the difference frequency is added to the present center frequency by an adder 44.
  • the frequency thus provided is set as a new center frequency in the radio frequency oscillator 17 through the center frequency I/F 30. Thus, the processing is terminated.
  • the center frequency is previously measured prior to the NMR imaging, the measurement free from position deviation can be preformed without using the magnetic field locking technique.

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  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Health & Medical Sciences (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Optics & Photonics (AREA)
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  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
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  • Magnetic Resonance Imaging Apparatus (AREA)
EP87115930A 1986-10-29 1987-10-29 Méthode pour corriger la déviation de position occasionnée par un changement du champ magnétique statique dans un appareil d'imagerie par RMN Expired - Lifetime EP0265956B1 (fr)

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EP93117910A EP0585973B1 (fr) 1986-10-29 1987-10-29 Méthode pour corriger les écarts de position occasionnée par un changement du champ magnétique statique dans un appareil d'imagerie par RMN

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JP61255666A JPS63109849A (ja) 1986-10-29 1986-10-29 Ｎｍｒイメ−ジング装置
JP255666/86 1986-10-29

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EP0265956A3 EP0265956A3 (en) 1989-08-16
EP0265956B1 EP0265956B1 (fr) 1994-06-01

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EP87115930A Expired - Lifetime EP0265956B1 (fr) 1986-10-29 1987-10-29 Méthode pour corriger la déviation de position occasionnée par un changement du champ magnétique statique dans un appareil d'imagerie par RMN

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EP0337588A2 (fr) * 1988-04-14 1989-10-18 The Regents Of The University Of California Imagerie par résonance magnétique compensée pour des variations erratiques de fréquence/phase dues à des variations erratiques de champs magnétiques au cours du processus de prise de données RMN
EP0391515A2 (fr) * 1989-04-05 1990-10-10 The Regents Of The University Of California Imagerie par résonance magnétique compensée pour des variations erratiques rapides dans le champ magnétique "statique" pendant une séquence unique de l'imagerie par résonance magnétique
DE4005675A1 (de) * 1990-02-22 1991-08-29 Siemens Ag Verfahren zur unterdrueckung von artefakten bei der bilderzeugung mittels kernmagnetischer resonanz
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EP0843203A1 (fr) * 1996-11-14 1998-05-20 Nashua Corporation Diffuseurs optiques obtenus par mélange à l'état fondu de matériels incompatibles
CN116559740A (zh) * 2023-03-16 2023-08-08 中国科学院精密测量科学与技术创新研究院 一种精确测量脉冲强磁场峰值场强分布的nmr方法与系统

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JPH05103768A (ja) * 1991-03-20 1993-04-27 Hitachi Ltd 磁気共鳴イメージング方法
DE4416363C2 (de) * 1994-05-09 1996-03-21 Siemens Ag Rekonstruktion von Bildern aus MR-Signalen in inhomogenen Magnetfeldern
DE19508238A1 (de) * 1995-03-08 1996-09-12 Siemens Ag Verfahren zur Magnetfeldstabilisierung bei einem Magneten für Kernspintomographieanlagen und Anordnung zur Durchführung des Verfahrens
DE19931210C2 (de) * 1999-07-06 2001-06-07 Siemens Ag Verfahren zur Korrektur von Artefakten in Magnetresonanzbildern
JP3951590B2 (ja) * 2000-10-27 2007-08-01 株式会社日立製作所 荷電粒子線装置
JP3992674B2 (ja) * 2003-09-25 2007-10-17 ジーイー・メディカル・システムズ・グローバル・テクノロジー・カンパニー・エルエルシー 磁気共鳴撮影装置
JP4619674B2 (ja) * 2004-03-24 2011-01-26 株式会社東芝 磁気共鳴イメージング装置
JP4798350B2 (ja) * 2005-10-26 2011-10-19 学校法人慶應義塾 磁気共鳴法を用いて試料中のプロトン性溶媒の挙動の分布を測定する測定装置、測定方法およびプログラム
JP6184050B2 (ja) * 2010-07-02 2017-08-23 東芝メディカルシステムズ株式会社 磁気共鳴イメージング装置
CN106680750B (zh) * 2016-12-29 2019-07-19 上海联影医疗科技有限公司 磁共振匀场图像获取方法、匀场方法及磁共振系统
US20240069134A1 (en) * 2021-02-24 2024-02-29 Case Western Reserve University System and method for b1-selective excitation for spatial localization in magnetic resonance imaging

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Cited By (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0337588A2 (fr) * 1988-04-14 1989-10-18 The Regents Of The University Of California Imagerie par résonance magnétique compensée pour des variations erratiques de fréquence/phase dues à des variations erratiques de champs magnétiques au cours du processus de prise de données RMN
EP0337588A3 (en) * 1988-04-14 1990-12-12 The Regents Of The University Of California Mri compensated for spurious nmr frequency/phase shifts caused by spurious changes in magnetic fields during nmr data measurement processes
EP0391515A2 (fr) * 1989-04-05 1990-10-10 The Regents Of The University Of California Imagerie par résonance magnétique compensée pour des variations erratiques rapides dans le champ magnétique "statique" pendant une séquence unique de l'imagerie par résonance magnétique
EP0391515A3 (fr) * 1989-04-05 1991-05-02 The Regents Of The University Of California Imagerie par résonance magnétique compensée pour des variations erratiques rapides dans le champ magnétique "statique" pendant une séquence unique de l'imagerie par résonance magnétique
DE4005675A1 (de) * 1990-02-22 1991-08-29 Siemens Ag Verfahren zur unterdrueckung von artefakten bei der bilderzeugung mittels kernmagnetischer resonanz
US5138259A (en) * 1990-02-22 1992-08-11 Siemens Aktiengesellschaft Method for suppressing image artifacts in a magnetic resonance imaging apparatus
DE4224237A1 (de) * 1991-07-31 1993-02-04 Hitachi Medical Corp Verfahren und vorrichtung zur selektiven anregung der kernspins bei abbildungen mittels magnetischer kernresonanz
US5386190A (en) * 1991-07-31 1995-01-31 Takeuchi; Hiroyuki Selective excitation method of nuclear spins in magnetic resonance imaging and MRI apparatus using the same
DE4224237C2 (de) * 1991-07-31 1998-06-10 Hitachi Medical Corp Verfahren und Vorrichtung zur selektiven Anregung eines Schnittbereichs bei der Bildgebung mittels NMR
EP0843203A1 (fr) * 1996-11-14 1998-05-20 Nashua Corporation Diffuseurs optiques obtenus par mélange à l'état fondu de matériels incompatibles
US5932342A (en) * 1996-11-14 1999-08-03 Nashua Corporation Optical diffusers obtained by fluid phase mixing of incompatible materials
CN116559740A (zh) * 2023-03-16 2023-08-08 中国科学院精密测量科学与技术创新研究院 一种精确测量脉冲强磁场峰值场强分布的nmr方法与系统
CN116559740B (zh) * 2023-03-16 2024-01-12 中国科学院精密测量科学与技术创新研究院 一种精确测量脉冲强磁场峰值场强分布的nmr方法与系统

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EP0265956B1 (fr) 1994-06-01
DE3752175T2 (de) 1998-11-05
DE3789933D1 (de) 1994-07-07
EP0585973A1 (fr) 1994-03-09
EP0585973B1 (fr) 1998-03-04
DE3752175D1 (de) 1998-04-09
JPH0580904B2 (fr) 1993-11-10
DE3789933T2 (de) 1994-09-08
EP0265956A3 (en) 1989-08-16
US4789833A (en) 1988-12-06
JPS63109849A (ja) 1988-05-14

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